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A uniform cylindrical block of length density and area of cross section floats in a liquid of density contained in a vessel . The bottom of the cylinder just rests on a spring of constant . The other end of the spring is fixed to the bottom of the vessel. A weight that may be placed on top of the cylinder such that the cylinder is just submerged in the liquid. Find the weight.
Applications of Bernoulli's Theorem

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Text: to zoom, left click on image and open in new tab For the next problems, consider the vector field 2y 2(x + 2y) 2y +y^2(2x + 2) a) Show that F is solenoidal by computing a vector potential for G, that is, a vector field G(G1, G2, G3) such that ∇ · G = F. Hint: your machine heart wants you to follow certain formulas assuming that G is 0. If you do that, you will be able to choose very simple constants of integration. (b) Let M be a surface whose boundary is given by c(t) = cos(t)sin(t), t ∈ [0,2]. Use your vector potential from (a) and Stokes's theorem to show that the flux of the current across our surface M is ∮ M F · dS = 0 A vector potential for F is not unique. However, a very important result in math known as Helmholtz's theorem states that, if F vanishes sufficiently fast as (x, y, z) → ∞ (our F does!), then F possesses a unique vector potential vanishing sufficiently fast as (x, y, z) → ∞ and satisfying the gauge condition ∇ · A = 0. Let's find this vector potential. If you didn't overcomplicate your life in (a), then the vector potential you found in (a) was A = (1, 0, 0) We know that G and A must differ by the gradient of a scalar function f: G = A + ∇f. Therefore, to find H, we just need to find this (mathematical) magical function f. Here's how we can find it: we apply the divergence operator to the expression above and we get that ∇ · G = ∇ · (A + ∇f) (*) where ∇^2f = ∇ · G is the Laplacian that you played with for Quiz 9 on 07/09. Equation (*) is a partial differential equation known as Poisson's equation. It's not obvious what its general solution should be (we're not that bad): (c) Compute ∇^2f, G and check that a solution to (*) is given by f = 2x^3y^2 + 22 [The function is pretty nasty so feel free to use WolframAlpha to compute the Laplacian of f. You really just have to enter ∇^2f] (d) We are finally ready to find our special vector potential!!!! Compute: H = G + ∇f.
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Question Text
A uniform cylindrical block of length density and area of cross section floats in a liquid of density contained in a vessel . The bottom of the cylinder just rests on a spring of constant . The other end of the spring is fixed to the bottom of the vessel. A weight that may be placed on top of the cylinder such that the cylinder is just submerged in the liquid. Find the weight.
TopicMechanical Properties of Fluids
SubjectPhysics
ClassClass 11
Answer TypeText solution:1
Upvotes82